Fluid transferring system and micropump suitable therefor

ABSTRACT

Disclosed herein is a micro fluid transferring system that comprises a micropump having a chamber, a first fluid transferring portion connected to the chamber, and a second fluid transferring portion connected to the chamber. This system is characterized in that at least one of the first and second fluid transferring portions comprises a pressure absorbing section for absorbing or alleviating a liquid vibrational pressure therein.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is based on Japanese Patent Application Nos.2002-088284, 2002-348285, and 2002-348286 filed with Japan Patent Officeon Mar. 27, 2002, Nov. 29, 2002, and Nov. 29, 2002, respectively, theentire content of which is hereby incorporated by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a fluid transferring system, andparticularly, to a fluid transferring system transferring a small amountof a fluid, e.g., liquid or gas, with high precision using a micropump.The present invention further relates to a micropump suitable for beingused in the fluid transferring system.

2. Description of the Related Art

Various kinds of micropumps transferring a small amount of liquid havebeen heretofore proposed. A micropump is incorporated in a fluidtransferring system for use in a chemical analysis or the like using asmall amount of liquid.

For example, a mocropump is disclosed in Japanese Patent Laid-OpenPatent Publication 2001-322099A, a chamber of which is connected to anexternal channel through an opening section. Furthermore, anotherdisclosure is given in an article entitled “AN IMPROVED VALVE-LESS PUMPFABRICATED USING DEEP REACTIVE ION ETCHING” appeared in Anders Olsson etal., MEMS'96 (IEEE), 479 to 484, in which two micropumps are installedin parallel and driven with a phase difference therebetween to therebycancel a mutual influence.

According to a construction of a fluid transferring system, a casearises where a characteristic thereof becomes deteriorated under aninfluence of an external flow channel. For example, in a case, apressure compressional wave produced by a vibration accompanying drivingof a micropump is reflected to interfere with the original waveaccording to a length and shape of the flow channel, thereby disablingachievement of a desired characteristic.

SUMMARY OF THE INVENTION

It is accordingly a technical object that the present invention seeks tosolve is to provide a fluid transferring system and/or micropump capableof improving fluid transferring efficiency thereof

Another technical object of the present invention is to provide a fluidtransferring system and/or a micropump capable of preventingdeterioration of a characteristic thereof.

Yet another technical object of the present invention is to provide afluid transferring system and/or a micropump capable of improving fluidtransferring efficiency thereof by giving multiple functions to themicropump.

A fluid transferring system reflecting an aspect of the presentinvention comprises: a micropump having a chamber; and first and secondfluid transferring portions respectively connected to the chambers,wherein at least one of the first and second transferring portions has apressure absorbing section for absorbing or alleviating a liquidvibrational pressure. Each of the first and second fluid transferringportions may be in a form of flow channel or a fluid reservoir, and maybe connected with the chamber through an opening section or closingvalve.

In the above construction, the liquid vibrational pressure produced incompany with driving of the micropump is absorbed or alleviated in thepressure absorbing section, thereby enabling decrease in the liquidvibrational pressure propagated from the pressure absorbing section.

With the above construction adopted, for example, in a case whereoccurrence of a turbulent flow is prevented by a liquid vibrationalpressure to thereby disable a desired characteristic to be obtained in afluid transferring system capable of transferring a liquid by producinga desired turbulent flow in a liquid spouting from an inlet of amicropump, an adverse influence of the liquid vibrational pressure canbe alleviated by absorbing or reducing the liquid vibratioal pressurewith the pressure absorbing section installed in the inlet side.Furthermore, by installing a pressure absorbing section on the outletside, a high frequency pulsating component is alleviated and asubsequent liquid stream can be of a near laminar flow. Alternatively, apressure absorbing section is installed in a propagation path of aliquid vibrational pressure to absorb or alleviate the liquidvibrational pressure, thereby enabling no return of a reflected wave tothe micropump or reduction in the reflected wave returning back to themicropump either.

Therefore, deterioration of a characteristic of a fluid transferringsystem can be prevented from occurring.

At least a portion of the pressure absorbing section is preferablydefined by a wall forming a portion of the at least one of the first andsecond fluid transferring portions and a thickness of the wall portionof the pressure absorbing section is thin enough to be deformable.

Since, in the above construction, a thickness of the wall is set thinenough to be deformable, the wall is deformed when a liquid vibrationalpressure acts thereon, thereby enabling absorption or alleviation of theliquid vibrational pressure through a change in volume.

A relation is preferably established in which the sum of the absolutevalues of a change in capacity (Cdr) of the at least one of the firstand second fluid transferring portions that comprises the pressureabsorbing sections caused by deformation when a unit pressure is appliedthereto; and change in volume (Cwr) of a liquid residing in the at leastone fluid transferring portion that comprises the pressure absorbingsection when the same unit pressure is applied thereto is larger thanthe sum of the absolute values of a change in capacity (Cdc) of thechamber when a unit pressure is applied thereto and a change in volume(Cwc) of the liquid in the chamber when the same unit pressure isapplied thereto. That is,|Cdr|+|Cwr|≧|Cdc|+|Cwc|  (1)

According to the above construction, a liquid vibrational pressureproduced in the chamber by driving of the micropump can be absorbed inthe flow channel or liquid reservoir including the pressure absorbingsection.

The pressure absorbing section is preferably present across a length ½or more times a wavelength of a pressure compressional wavecorresponding to a driving cycle of the micropump in a fluidtransferring direction of the at least one of the first and second fluidtransferring portions. A change in capacity of the pressure absorbingsection when a unit pressure is applied to the pressure absorbingsection is larger than a change in volume of a liquid in the pressureabsorbing section when the same unit pressure is applied to the liquid.

With the above construction adopted, propagation of a pressurecompressional wave in which a portion to propagate forward and a portionto propagate backward are alternately present repeatedly, with eachportion having one half wavelength, can be blocked or reduced in thepressure absorbing section.

Furthermore, a fluid transferring system reflecting another aspect ofthe present invention comprises: a micropump having a chamber; and firstand second fluid transferring portions respectively connected to thechamber, wherein at least one of the first and second fluid transferringportions comprises a pressure reflecting section for reflecting a partof a pressure compressional wave propagating in a direction of movingaway from the chamber, to the chamber side. Each of the first and secondfluid transferring portions may be in a form of flow channel or a fluidreservoir, and may be connected with the chamber through an openingsection or closing valve.

According to the above construction adopted, the reflected wave directedto the chamber side can be caused to properly interfere with an originalwave propagating toward the reflecting section from the chamber so asnot to cause an adverse influence by interference and furthermore tothereby use the interference intentionally to improve a characteristicof the micropump.

Therefore, it can prevent the deterioration of characteristics of afluid transferring system.

The pressure reflecting section preferably includes: a portion of whichan effective acoustic impedance is discontinuous or a flow channel bendswith a sharp angle.

In the above construction, reflection of a pressure compressional waveoccurs in a portion where an effective acoustic impedance isdiscontinuous or a flow channel bends with a sharp angle. Herein, aneffective acoustic impedance can be calculated using an acousticcapacitance in consideration of not only a change in volume of a fluiditself, but also a change in capacity of a space confining the liquid,that is a flow channel or the like.

Moreover, a fluid transferring system reflecting still another aspect ofthe present invention comprises: a micropump having a chamber to which afirst opening section and a second opening section are formed, wherein,when a pressure in the chamber is raised or lowered, a change percent inflow channel resistance at the first opening section is smaller than achange percent in flow channel resistance at the opening section; andfirst and second fluid transferring portions respectively connected tothe chamber though the first and opening sections, respectively, whereinthe first fluid transferring portion has a reflecting section forreflecting a part of a pressure compressional wave propagating in adirection of moving away from the chamber, to the chamber side. Adistance in the flow channel or liquid reservoir to the reflectingsection from the one opening section is ½ or less times a wavelength ofa pressure compressional wave corresponding to a driving cycle of themicropump.

In the fluid transferring system of the above construction, since achange percent in flow channel resistance at the one opening is smallerthan a change percent in flow channel resistance at another openingsection, a ratio of a flow in passage between the respective openingsections is different according to whether a pressure in the chamber ison the rise or fall and liquid transfer is thereby realized using thenature of the system.

In the above construction, in order to obtain a good liquid transfercharacteristic, a flow channel resistance at the one opening sectiondesirably changes in value by the lowest possible amount. In order torealize the condition, it is preferably required to prevent a pressurefrom changing largely at the one opening. To be concrete, it ispreferably required that a distance from the one opening section to thereflecting section is set to cause the pressure compressional wavepropagating toward the reflecting section from the one opening sectionto cancel the reflecting wave reflected toward the one opening sectionin the reflecting section while avoiding a value in the vicinity of Ntimes (N=1, 2, . . . ) a half wavelength of a pressure compressionalwave. When N becomes larger, however, not only does an effect to canceleach other decrease because of attenuation of the reflecting wave, butalso a result different from the intention altogether would be easilyobtained if a phase difference is shifted because of a slight designerror or external disturbance. On the other hand, when a distance fromthe one opening section to the reflecting section is ½ or less times awavelength of the pressure compressional wave, attenuation of thereflected wave is small to thereby increase a canceling effect, therebyenabling a target result to be obtained even in the presence of designerror and external disturbance.

When a fluid transferring system is constructed with plural micropumpsin connection so as to include at least one of the above contrivances ofconstruction, mutual interferences of the micropumps can be preventedfrom occurring; therefore, a high characteristic of the system can bestably obtained. To be concrete, the construction is as follows.

The chambers of the above micropumps are arranged in parallel to eachother. The flow channels or the liquid reservoirs communicating with therespective chambers are merged.

According to the above construction, for example, in a case where pluralmicropumps are adopted in order to increase a flow rate, a desiredcharacteristic can be attained.

As a different construction, the chambers of the plural micropumps arepreferably arranged in series with each other. Adjacent ones of thechambers are connected to each other through at least one of theopenings section (or the closing valves), the flow channels and theliquid reservoirs.

According to the above construction, for example, in a case where pluralmicroumps are employed in order to raise a pressure, a desiredcharacteristic can be obtained.

Furthermore, the present invention provides a fluid transferring systemof the following construction in order to solve the above technicalproblems.

The fluid transferring system is constructed so that chambers of pluralmicropumps are arranged in series with each other. A length of aconnecting section connecting adjacent ones of the chambers is shorterthan a half wavelength of a pressure compressional wave corresponding toa driving cycle of the micropumps. Adjacent ones of the chambers aredriven in respective different driving waveforms or with a differentphase difference therebetween.

In the above construction, a length of a connecting section is designedto be shorter than ½ times a wavelength of a pressure compressional waveto thereby cause a reflecting wave and an original wave to properlyinterfere with each other so as not to produce an adverse influence dueto interference, or furthermore, interference is intentionally used soas to improve a fluid transferring characteristic of a micropump.Furthermore, adjacent chambers are driven in respective differentdriving waveforms or with a phase difference therebetween not only so asto prevent resonance between adjacent micropumps, but also so as tocause proper interference between pressure compressional waves producedby driving respective micro pumps, thereby enabling intentional use ofthe interference for improvement on fluid transferring characteristic.

Therefore, a characteristic of a fluid transferring system can beprevented from deteriorating.

Furthermore, a fluid transferring system reflecting still another aspectof the present invention is of a type in which chambers of pluralmicropumps are arranged in series with each other and a length of aconnecting section connecting adjacent ones of the chambers is ¼ or moretimes a wavelength of a pressure compressional wave corresponding to adriving cycle of the micropumps.

In a case where plural micropumps are connected in series with eachother, a length of a connecting section between chambers of themicropumps shorter than ¼ times a wavelength of a pressure compressionalwave cannot be used for improvement on a fluid transferringcharacteristic since a reflected wave does not cancel an original wavein interference, but to the contrary, a possibility arises that theshorter distance exerts an adverse influence. According to the aboveconstruction, since a length of the connection section is ¼ or moretimes a pressure compressional wave, the interference between thereflected wave and the original wave can prevent an adverse influence ofthe interference and can be intentionally used to improve acharacteristic.

Therefore, a characteristic of a fluid transferring system can beprevented from deteriorating.

A micropump reflecting still another aspect of the present inventioncomprises: a chamber; a first opening section including a plurality ofsub-opening sections, each of the sub-opening sections being forconnecting the chamber with a first fluid transferring portion, thesub-opening sections having an effective sectional area smaller thanthat of the first fluid transferring portion and showing, as a whole, afirst flow channel resistance that changes depending on change indifferential pressure between the chamber and the first fluidtransferring portion; and a second opening section for connecting thechamber with a second fluid transferring portion, the second openingsection having an effective sectional area smaller than that of a thesecond fluid transferring portion, the second opening section showing asecond flow channel resistance that changes depending on change indifferential pressure between the chamber and the second fluidtransferring portion, wherein the differential pressure dependency ofthe first flow channel resistance is smaller than that of the secondflow channel resistance.

In a case where the micropump further comprises another openingsection(s) for connecting the chamber with another fluid transferringportion(s), the differential pressure dependency of the first channelresistance is preferably smaller than those of the remaining ones.

Furthermore, in the sub-opening sections of the first opening section,the minimum of ratios of flow channel lengths to sectional areas of therespective sub-opening sections is set to be larger than a ratio of flowchannel length to the sectional area of the second opening section. Withthe construction in which the chamber communicates with the first fluidtransferring portion through the plurality of sub-opening sections,reduction occurs in pressure dependency as a whole of the first openingsection thereby increase a difference in pressure dependency between thefirst and second opening sections. By doing so, improvement is achievedon a flow rate characteristic and efficiency of a pump.

A fluid control system reflecting still another aspect of the presentinvention comprises: a chamber; a first opening section for connectingthe chamber with a first fluid transferring portion, the first openingsection having an effective sectional area smaller than that of thefirst fluid transferring portion and showing a first flow channelresistance that changes depending on change in differential pressurebetween the chamber and the first fluid transferring portion; a secondopening section for connecting the chamber with a second fluidtransferring portion, the second opening section having an effectivesectional area smaller than that of a the second fluid transferringportion, the second opening section showing a second flow channelresistance that changes depending on change in differential pressurebetween the chamber and the second fluid transferring portion; and athird opening section for connecting the chamber with a third fluidtransferring portion, the third opening section having an effectivesectional area smaller than that of a the third fluid transferringportion, the third opening section showing a third flow channelresistance that changes depending on change in differential pressurebetween the chamber and the third fluid transferring portion, whereinthe differential pressure dependency of the first flow channelresistance is different from those of the second and third flow channelresistances.

In the above mentioned structure, the differential pressure dependencyof the second flow channel resistance is preferably different from thatof the third flow channel resistance.

Furthermore, in a case where the differential pressure dependency of thefirst opening section is smaller than those of the second and thirdopening sections, the first opening section may preferably comprise aplurality of sub-opening sections each of which connects the chamberwith the first fluid transferring portion.

Moreover, at least one of the first sub-opening sections preferably hasa uniform flow channel section and is larger in a ratio of a length offlow channel to a sectional area thereof than any one of those of thesecond sub-opening sections and the third opening section.

Such a micro-fluid system is used in a manner such that a change ratioin flow channel resistance is caused to be altered in value according towhether a volume of the chamber increases or decreases under control ofa driving voltage waveform given to the actuator to thereby transport afluid to the opening sections or the opening section groups at flowrates and in a direction according to a value of flow channel resistanceof each of them to thus merge fluid flows or divide a fluid flow.

BRIEF DESCRIPTION OF THE DRAWINGS

These and other objects, advantages, and features of the presentinvention will become apparent from the following description thereoftaken in conjunction with the accompanying drawings in which:

FIG. 1 is a sectional view of a micropump;

FIG. 2 is a plan view of a fluid transferring system of a firstembodiment reflecting aspects of the present invention;

FIG. 3 is a plan view of a fluid transferring system of a firstmodification of the first embodiment;

FIG. 4 is a plan view of a fluid transferring system of a secondmodification of the first embodiment;

FIGS. 5( a) and (b) are sectional views of a micropump of a thirdmodification of the first embodiment;

FIG. 6 is a plan view of a fluid transferring system of a secondembodiment reflecting aspects of the present invention;

FIG. 7 is a plan view of a fluid transferring system of a firstmodification of the second embodiment;

FIG. 8 is a plan view of a fluid transferring system of a secondmodification of the second embodiment;

FIG. 9 is a plan view of a fluid transferring system of a thirdembodiment reflecting aspects of the present invention;

FIG. 10 is a plan view of a fluid transferring system of a firstmodification of the third embodiment;

FIG. 11 is a plan view of a fluid transferring system of a secondmodification of the third embodiment;

FIG. 12 is a plan view of a fluid transferring system of a thirdmodification of the third embodiment;

FIGS. 13( a) and 13(b) are a plan view and driving voltage waveforms ofa fluid transferring system of a fourth modification of the thirdembodiment;

FIGS. 14( a) and 14(b) are a plan view and driving voltage waveforms ofa fluid transferring system of a fifth modification of the thirdembodiment;

FIG. 15 is a plan view of a fluid transferring system of sixthmodification of the third embodiment;

FIG. 16 is a plan view of a fluid transferring system of seventhmodification of the third embodiment;

FIGS. 17( a) and 17(b) are graphs of a displacement behavior and adriving voltage of a micropump of FIG. 1;

FIGS. 18( a) and 18(b) are other graphs of a displacement behavior and adriving voltage;

FIGS. 19( a) and 19(b) are still other graphs of a displacement behaviorand a driving voltage;

FIG. 20( a) and FIG. 21( a) are graphs showing example waveforms ofdriving voltage of a piezoelectric element;

FIG. 20( b) and FIG. 21( b) are model graphs showing flow rates obtainedby a pumping action according to voltage waveforms shown in FIG. 20( a)and FIG. 21( a);

FIG. 22( a) and FIG. 22( b) are graphs showing examples of flow channelresistance characteristics at an opening sections;

FIG. 23 is an enlarged view showing an opening section group 24 of amicropump;

FIG. 24 is a view showing an example of an opening section group 24provided with three opening sections;

FIG. 25 is a model plan view showing a construction of a thirdmodification of the first embodiment of the present invention;

FIG. 26 and FIG. 27 are a model plan view and a model front sectionalview showing a construction of a fluid transferring system of a fourthembodiment of the present invention;

FIG. 28 is a graph showing a flow channel resistance characteristic ofeach opening section in a micropump of the fourth embodiment;

FIG. 29 and FIG. 30 are graphs showing example of a driving voltagewaveforms of a piezoelectric element;

FIG. 31 is a graph showing an appearance of change in volume of achamber 20 according to a driving voltage;

FIG. 32 is a model plan view showing a construction of a fluidtransferring system of a first modification relating to the fourthembodiment of the present invention; and

FIG. 33( a) to FIG. 33( c) are another examples to which fluidtransferring system of the present invention is applicable.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Description will be given of examples as embodiments of the presentinvention based on FIG. 1 to FIGS. 19( a) and 19(b). Note that similarconstituents in the figures are indicated with the same symbols.

Fist of all, description will be given of a fluid transferring system ofthe first example of a first embodiment with reference to FIG. 1 to FIG.5 and FIG. 17( a) to FIG. 19( b).

FIG. 1 is a sectional view of a micropump 10 used in a fluidtransferring system. FIG. 2 is a plan view of the fluid transferringsystem.

In the fluid transferring system, a base plate 12 and a thin plate 14are bonded together. The base plate 12 has a surface on which there areformed: recesses serving as a chamber 20 and a liquid reservoir 30; andslits serving as first and second opening sections 22 and 24 and a flowchannel 34, and the thin plate 14 working as a vibrating plate is bondedonto the surface. A through hole 32 for supplying a liquid is formed inthe thin plate 14 and the through hole 32 communicates with the liquidreservoir 30. A piezoelectric element 16 is fixed on the top surface ofthe thin plate 14 oppositely to the chamber 20. The piezoelectricelement 16 and the thin plate 14 constitutes of an actuator of amonomorph structure and a voltage is applied to the piezoelectricelement 16 from a driving circuit 18 to thereby bend the actuator to acurved form.

The chamber 20 is connected to the liquid reservoir 30 and the flowchannel 22 through the first opening section 22 and the second opening24, respectively. The liquid reservoir 30 has a width wider and a volume(or a capacity) larger as compared with the chamber 20, the flow channel34. The first opening section 22 is formed so that a change percent inflow channel resistance thereof according to a differential pressurebecomes larger as compared with the second opening section 24.

Note that the first opening section 22 and the second opening section 24are not required to be formed each as a single narrow flow channel, but,for example, like a micropump 10 a in a first modification of thepresent embodiment shown in FIG. 3, the second opening section may alsobe constituted of a plurality of flow channels 24 a and 24 b. This maybe applied to the first opening section in a similar manner.

The micropump 10 uses a mechanism of a combination of the thin plate 14and the piezoelectric element 16 that is subjected to a curveddeformation in a unimorph mode to increase or decrease a volume (or acapacity) of the chamber 20 and to change a pressure in the chamber 20.At this time, a liquid is transferred using a nature that change ratesin flow channel resistance of the first opening section 22 and thesecond opening section 24 are different according to a pressure on therise or fall.

That is, decrease in volume of the chamber 20 pushes out the liquid inthe chamber 20 through the first and second opening sections 22 and 24.When a volume of the chamber 20 restores to the original one, the liquidis sucked into the chamber 20 through the first and second openingsections 22 and 24. By repeating the process, the liquid can betransferred in a desired direction in the following manner.

If a flow-out amount of the liquid flowing out from the chamber 20through the first and second opening sections 22 and 23 are V₁₁ and V₂₁,and the flow-in amount into the chamber 20 through the first and secondopening sections 22 and 24 are V₁₂ and V₂₂ by definition, the followingequation is given:V ₁₁ +V ₂₁ =V ₁₂ +V ₂₂  (2)

As described above, here, the first opening section 22 is formed so thata change rate in flow channel resistance according to a differentialpressure is larger as compared with the second opening section 24. Inother words, the differential pressure dependency of the flow channelresistance of the first opening section 22 is larger than that of thesecond opening section 24.

Therefore, for example, when a volume of the chamber 20 is rapidlyreduced to thereby relatively increase a differential pressure and thena volume of the chamber 20 is gradually restored to thereby relativelydecrease a differential pressure, the following relation is established:V₁₁<V₁₂  (3)

Furthermore, from the equation (2) and the relations (3), the followingrelation is given:V₂₁>V₂₂  (4)

As can be understood from the relations (3) and (4), the liquid istransferred in the forward direction in FIG. 1 as a whole.

To the contrary, when a volume of the chamber 20 is gradually decreasedto make a differential pressure relatively small, and then, a volume ofthe chamber 20 is rapidly restored to thereby relatively increase adifferential pressure, the liquid is transferred to in the reversedirection in FIG. 1.

Description will be given of one concrete example below. Aphotosensitive glass of 500 μm in thickness is adopted as the base plate12, on which etching is applied to form recesses of the chamber 20 andthe liquid reservoir 30, and slits of the first and second openingsections 22 and 24 and the flow channel 34, all reaching to 100 μm indepth. The first opening section 22 has dimensions of 100 μm in depth,25 μm in width and 20 μm in length. The second opening section 24 hasdimensions of 100 μm in depth, 25 μm in width and 150 μm in length. Themain part of the liquid reservoir 30 is of a rectangular parallelepipedhaving dimensions of 100 μm in depth, 1.2 mm in width and 4.0 mm inlength. The liquid reservoir 30 is formed so as to increase its width bythe angle of 45 degrees, leftward and rightward, in to the interiorstarting at the opening section 22. The flow channel 34 has dimensionsof 100 μm in depth, 150 μm in width and about 15 mm in length. The thinplate 14 is a glass plate of 50 μm in thickness, on the top surface ofwhich the piezoelectric element 16 of 50 μm in thickness made of PZT(lead zirconate titanate) ceramic is fixed with an adhesive agent. Notethat when a voltage of 30 V is applied to the piezoelectric element 16,a displacement (the maximum recess) is 80 nm, which produced a pressureof 0.4 MPa in water filling the chamber 20.

Then, description will be given of a driving voltage waveform applied tothe piezoelectric element 16 of the micropump 10.

The micropump 10 is required to drive the actuator section 15 (as shownin FIG. 1, the portion of the thin plate 14 facing the chamber 20 andthe piezoelectric element 16 fixed thereon) to increase or decrease avolume of the chamber 20 so that a displacement speed in vibrationthereof is different according to a volume of the chamber 20 when itincreases or decreases.

As for a vibration of the actuator section 15, its vibrational behavioris determined by a vibrational mode in which a vibration of a flow ofthe liquid resonates with a vibration of the actuator section 15(hereinafter referred to as natural vibration) as a major factor. When avoltage is applied to the piezoelectric element 16 to vibrate theactuator section 15, the actuator section 15 can be efficiently drivenby applying a driving voltage waveforms so as to attain a desiredvibrational behavior paying attention to a cycle of the naturalvibration.

A cycle of the natural vibration (or a natural vibration cycle) can beexpressed using the following 4 acoustic factor components:

-   -   (a) an acoustic capacitance of the actuator section 15: Cp,    -   (b) an acoustic capacitance of a liquid in the chamber 20: Ca,    -   (c) an inertance of the first opening section 22: Mi and    -   (d) an inertance of the second opening section 24: Mo.

The “acoustic capacitance” here corresponds to compression (ordeformation) in volume per a unit pressure. As for (a), deformation ofthe base plate 12 can be neglected and the capacitance can be calculatedby obtaining only deformation in volume of the actuator section 15 whena unit pressure is applied on the inner surface of the chamber 20. Asfor (b), the capacitance can be calculated from a decrease in volumewhen a unit pressure is applied to the entire liquid in the chamber 20.Alternatively, if a density of the liquid is p, an acoustic velocity inthe liquid is v and a volume of the chamber 20 is W by definition, thecapacitance Ca is obtained by the following equation:Ca=W/(ρv ²)  (5)

If the base plate 12 is an elastic body such as made of a resin,deformation of the elastic body should be considered in the calculationof (a).

The “inertance” corresponds to a coefficient of inertia when a liquid inthe flow channel is pushed out by a unit pressure. An inertance M can becalculated from an acceleration α at a pressure P with the followingequation:M=P/α  (6)

Or, if a mass of a liquid in the flow channel is m and a sectional areaof the flow channel is S by definition, the inertance M can becalculated with the following equation:M=m/S ²  (7)

As for a flow channel whose sectional area is not uniform, it ispreferably required to use an integral with respect to a distance in thelongitudinal direction.

Note that in a case where the first or second opening section 22 or 24is constituted of a plurality of flow channels, it is preferable totreat these flow channels as parallel flow channels and to use aninertance of the parallel flow channels for this calculation. Forexample, if, as shown in FIG. 3, two flow channels 24 a and 24 bcorrespond to the second opening section, the flow channels 24 a and 24b are in a parallel relationship, so an inertance of the entire secondopening sections 24 a and 24 b is an reciprocal of the sum ofreciprocals of inertances of individual flow channels 24 a and 24 b.

A natural vibration cycle T is given with the following equation usingacoustic capacitances Cp and Ca and inertances Mi and Mo:T=2π((Cp+Ca)×Mo×Mi/(Mo+Mi))  (8)

The natural vibration cycle T of this vibrational mode, however, is insome case shifted in value by factors under influences of flow channelsconnected to the micropump 10, a mass component of the actuator 16 andothers. An actual value has a possibility to be shifted by a factor ofthe order in the range of from 0.5 to 2 times from a calculated valuewith the equation (8).

Note that while there is a natural vibration in a general sense derivedfrom a mode in which the actuator section 15 vibrates singly by itself,a vibrational mode based on an interaction between the micropump 10 andexternal flow channels connected to the micro pump 10 and others, avoltage driving waveform herein is determined paying attention only to avibration of the actuator section 15 and a vibration of a flow of theliquid resonating with a vibration of the actuator section 15.

Then, in FIGS. 17( a) to 19(b), there are shown examples of drivingvoltage waveforms for achieving desired vibrational behaviors of theactuator section 15. The following examples are presented by way ofexamples only in all respects, but any of driving voltage waveforms canbe used without causing a problem as far as a vibrational velocity ofthe actuator section 15 is different according to a volume of thechamber 20 when it increases or decreases. For example, one cycleincluding an increase in volume and a decrease in volume of the chamber20 may be realized by a combination of plural driving voltage waveforms.Alternatively, while the case is exemplified where the piezoelectricelement 16 is used in order to deform the chamber 20, there may be useda driving mechanism other than it (for example, an electrostaticactuator, a magnetostrictive element, shape memory alloy or the like).

FIGS. 17( a) and 17(b) show driving voltage waveforms 91 a and 91 bdifferent in rise time T_(R) and fall time T_(F), and waveforms 90 a and90 b of displacement behaviors (deflections) of the piezoelectricelement 16 corresponding to the driving voltage waveforms. The drivingvoltage waveform 91 a in driving in a forward direction has a relationof T_(R)<T_(F) while the driving voltage waveform 91 b in driving in areverse direction has a relation of T_(R)>T_(F).

At least one of the rise time T_(R) and fall time T_(F) is preferably anatural vibration cycle T or more. This is because in a case where avoltage applied to the piezoelectric element 16 gradually changes over atime longer than a cycle of the natural vibration, a vibrationalbehavior of the actuator section 15 is harder to receive an influence ofthe natural vibration; therefore, the vibrational behavior is easier tofollow a voltage waveform and as a result, the vibrational behavior ofthe actuator 15 is controlled with ease.

Note that while the driving voltage waveforms 91 a and 91 b are of atrapezoid, plateaus 92 a and 92 b at the tops thereof are not alwaysnecessary.

Driving voltage waveforms 95 a and 95 b and waveforms 94 a and 94 b ofdisplacement behaviors of the piezoelectric element 16 of FIGS. 18( a)and 18(b) are cases where the driving voltage waveforms 95 a and 95 bare rounded with time constants τ₁ and τ₂ determined by a capacitance,an electric resistance and others. For example, such deformation of thewaveforms can be realized by differentiating a wiring resistance of aswitching circuit in between charging and discharging to change timeconstants τ₁ and τ₂ or by incorporating a rectifying element such as adiode and a non-linear element in a driving circuit or wiring todifferentiate a charge time and discharge time from each other.Furthermore, by using a capacitance variable with respect to a voltagesuch as an electrostatic actuator, the time constants τ₁ and τ₂ changeswith time, so, as a result the rounded driving voltage waveforms 95 aand 95 b can be realized.

In FIGS. 19( a) and 19(b), there are shown driving voltage waveforms 97a and 97 b using pulse waveforms 98 a and 98 b such as a rectangularwave, and waveforms 96 a and 96 b of displacement behaviors of thepiezoelectric element 16. A driving cycle T₂ of the driving voltagewaveforms 97 a and 97 b is slightly shifted from a natural vibrationcycle T. If the range of the driving cycle T₂ is about ½ time to 2 timesa natural vibration cycle T, this method is effective. This is a drivingmethod in which a phenomenon is used that if duty ratio (T₁/T₂) of thedriving pulses 98 a and 98 b is changed, changes occur in lengths of arise time and a fall time in displacement of the piezoelectric element16. Liquid transfer in two directions can be realized by using a naturereversing a relationship in length between a rise time and a fall timeat a duty ratio of 50% as a boundary. Note that it is not necessary thatthe pulse waves 98 a and 98 b are of rectangular, but may be of atriangular, trapezoidal or the like.

Then, description will be given of absorption of pulsation pressuresgenerated by the micropump.

As shown in FIG. 1, the top wall of the liquid reservoir 30 is made ofthe thin plate 14. This construction can be applied to alleviate thepulsation in pressure of a liquid spouting from the first openingsection 22 outside the chamber 20, thereby enabling a stablecharacteristic to obtained.

In order to discuss a characteristic of pressure absorption in terms ofnumerical sense, a concept may well be used that as described above, “anacoustic capacitance C=compression (or deformation) in volume per a unitpressure.” It is considered that with a larger value, a higher degree ofpressure absorption for alleviation is realized since more of a instantchange in pressure is absorbed by deformation (compression). Note thatthe capacitance should be evaluated with the sum of two components of afactor associated with compressibility of a liquid (Cw) and a factorassociated with deformation of the thin plate 14 on the top wall (Cd).

Herein, if a density of a liquid is p and an acoustic velocity (apropagation velocity of a plane pressure wave) is v and a volume is X bydefinition, Cw can be expressed by the following equation:Cw=X/(ρ×c ²)  (9)

Furthermore, as for deformation of the thin plate 14 of the top wall,there can be used an equation of a known “an iso-pressure strain in aplate of a constant thickness with fixed 4 sides thereof.” If as to theplate, a thickness is t, a width is w and Young's modulus is E bydefinition, Cd can be expressed by the following equation:Cd=α×L×w ⁵/(2×E×t³)  (10)

Herein, α is a dimensionless constant and when a ratio of a width and alength is 2 or more, α≈0.0028.

To be concrete, if the sum of the absolute values of capacitance valuesC of the liquid reservoir 30 is larger than that of the chamber 20, theliquid reservoir 30 plays a role as a pressure absorbing section. Thisis because, since a pressure compressional wave is produced bydeformation of the wall surface of the chamber 20, a deformation involume caused by the pressure in a portion harder (smaller incapacitance) than the wall of the chamber 20 is equal to or smaller thana volume vibrational amount produced in the chamber 20, which makes theportion improper as a pressure absorbing section.

In the above concrete example, since the liquid reservoir 30 is largerin volume than the chamber 20 by a factor of 3 or more-fold, Cw is threeor more-fold. Moreover, since a width of the liquid reservoir 30 portionof the thin plate 14 is larger than that of a portion of the thin plate14 of the chamber 20 by a factor of 2.4-fold and does not disturb adisplacement of the thin plate 14, Cd is about 80 or more-fold.Therefore, since the total capacitance of the liquid reservoir 30 issufficiently larger than a capacitance of the chamber 20, a sufficienteffect can be expected.

While in this embodiment, one pressure absorbing section (the liquidreservoir 30) is installed at a position very close to an outlet of thefirst opening sections 22, even if at least one of the position and thenumber of the pressure absorbing sections is different from thisembodiment, the effect is still ensured. Moreover, a pressure absorbingsection may be at some mid point in the flow channel 34 in the secondopening section 24 side.

Note that as for the micropump 10 shown in FIGS. 1 and 2, it is verysignificant that the liquid reservoir 30, which is a pressure absorbingsection, is installed at the position immediately close to the outlet ofthe first opening section 22.

This is because in the micropump 10 of this type, a characteristic isused that a flow channel resistance of the first opening section 22increases under a high pressure by an effect of a turbulent flowproduced in the vicinity of the first opening section 22, therefore, anecessity arises for controlling a value of differential pressure acrossboth ends of the first opening section 22 so as to achieve a targetvalue with good precision. Therefore, again this is because as for apressure (in the liquid reservoir 30) at a position very close to theoutlet of the first opening section 22, a necessity arises for holdingthe pressure at the outlet to a value sufficiently lower than a peak ofan inner pressure of the chamber 20 at all times.

In other words, the micropump 10 of this type is driven by use of alarge change in flow channel resistance caused by the presence orabsence of a turbulent flow produced in the vicinity of the firstopening section 22. While a case occurs where no desired turbulent flowis produced under an influence of pulsation during when the micropump 10is driven, the desired turbulent flow can be produced if the liquidreservoir 30 is constructed so as to work as an pressure absorbingsection to thereby exclude an influence of the pulsation, therebyenabling improvement on characteristic and stabilization thereof.

The top wall of the flow channel 34 is made of the thin plate 14. Sincethe flow channel 34 is narrower in width as compared with the reservoir30, the flow channel shows no pressure absorbing characteristic as largeas the liquid reservoir 30, but shows the following effect.

That is, in a case where the flow channel 34 is long, motion of a liquidin the second opening section 24 receives directly an influence of aninertia force of the liquid of the flow channel 34. Hence, a vibrationresponsive to a driving cycle of the pump 10 is obstructed to thereby,enable expectation to prevent a problem of disabling normal liquidtransfer due to the pulsation beforehand.

To be detailed, the inertia force of a flow channel is proportional toan inertance (an acoustic inertia coefficient) M. An inertance M, as isdescribed in connection with the equation (7), is proportional to alength of a flow channel and inversely proportional to the square of asectional area. Therefore, with a shallower flow channel, a narrowerwidth thereof and a smaller sectional area thereof, and furthermore witha longer flow channel, the inertance is easier to receive an influenceof an inertia of the flow channel. An inertia force is also proportionalto an acceleration, however. Therefore, while a prescribed pressure isapplied to a uniform flow throughout all the flow channel covering allthe flow channel, as to propagation of a high frequency vibration, onlyan inertia force for a half length of the wavelength effectively works.This is because as to propagation of a high frequency vibration, thereare alternately present a portion with a half wavelength to propagateforward and a portion with a half wavelength to propagate backward ineach one wavelength.

A wavelength in propagation of a high frequency vibration in the flowchannel can be expressed using the above acoustic capacitance C and aninertance M. If a capacitance per a unit length is Ca and an inertanceper a unit length is Ma by definition, a length of a half wavelength Lhof a vibration with a vibrational cycle T is given by the followingequation:Lh=T/√(Ma×Ca)  (11)

As can be understood from the equation (11), with a larger capacitanceper a unit length: Ca, a length: Lh for which an inertance effectivelyworks for a high frequency vibration decreases (that is, an effectiveinertance decreases). In order to realize “a construction of pressureabsorption”, a width of the flow channel 34 is increased and the thinplate 14 of the top wall is thinned to increase a capacitance, therebyenabling expectation of the above effect. Note that, this method is alsoa useful means in addition to solution of the above object for a casewhere design is used in a system of a good response even with aconstruction having a long flow channel or for a case where pulsationvibration is desired to intentionally propagate to a remote area.

Note that the effect of the present embodiment is not limited to themicropumps 10 of the type shown in FIG. 1, but generally is effectivefor all the types of micropumps accompanying pulsation in liquidtransfer.

For example, the effect of the present embodiment is especiallyeffective for a valveless micropump such as a micropump 40 of a typecalled “nozzle/diffuser type,” as shown in the top view of FIG. 4,having inlet/outlet 42 and 44 each having a widening shape as openingsections, and using a larger flow channel resistance in a wideningdirection at all times. The micropump 40 of FIG. 4, similar to themicropump 30 shown in FIGS. 1 and 2, a piezoelectric element 48 is ACdriven to transfer a liquid in the chamber 46.

Furthermore, since in a micropump 50 of a type, as shown in a sectionalview of FIGS. 5( a) and (b), in which a liquid is transferred in companywith opening and closing of valves 52 and 54 as well, it is expectedthat in a driving at a higher velocity, a liquid transfer amount per onecycle is affected by pulsation with more of ease; therefore, the aboveeffect is considered to be effective. A micropump 50 of FIGS. 5( a) and(b) drives at prescribed timings piezoelectric elements 52 a and 54 aopening or closing valves 52 and 54 in synchronization with apiezoelectric element 56 a facing a chamber 56. For example, in a statewhere the valve 52 is closed as shown in FIG. 5( a), the chamber 56 isdeformed to pressurize and to push out the liquid to the flow channel 34from the chamber 56 as shown with an arrow mark 50 a. Then, in a statewhere the valve 54 is closed as shown in FIG. 5( b), the chamber 56, asshown with an arrow mark 56 t, is restored to an original state whilereducing a pressure therein and to suck the liquid from the liquidreservoir 30 as shown with an arrow mark 50 b. The operations arerepeated thereafter.

Then, description will be given of the second embodiment with referenceto FIGS. 6 to 8.

While a fluid transferring system shown in FIG. 6 is constructed in analmost similar way to the first embodiment shown in FIGS. 1 and 2,dissimilar to the first embodiment, a pressure absorbing section 60 isinstalled at some mid point of the flow channel 34 connected to thesecond opening section 24. The top wall of the pressure absorbingsection 60 is made of thin plate 14, as in the first embodiment. Since awidth of the pressure absorbing section 60 is wider than the flowchannel 34, the thin plate 14 of a portion facing the pressure absorbingsection 60 is deformed into deflection by a pressure with more of ease.A capacitance (Cd) of the pressure absorbing section 60 due todeformation of the thin plate 14 is proportional to a width w to thefifth power as shown in the equation (10),so the width wider by apercent of the order of, for example, 20% only, the capacitanceincreases by a factor of about 2. 5-fold. While, in fact, the effectshould be evaluated using the sum including a capacitance (Cw) due tocompression of the liquid, there is a case where the widening to thislevel alone sufficiently works as a pressure absorbing section.

In this pressure absorbing section 60, not simply is a pressureabsorbing effect is exerted, but there is available therein acharacteristics to reflect a high frequency compressional wave. To beconcrete, a reflection occurs in a position where an effective acousticimpedance changes such as the boundaries 61 a and 61 b between the flowchannel 34 and the pressure absorbing section 60. Reflection can occurin not only a portion where an acoustic impedance increases, but also aportion where an acoustic impedance decreases.

If an acoustic impedance in a portion (portion of La) prior to areflecting section 61 a is Za and an acoustic impedance in a portion(portion of Lb) ahead of the reflecting section 61 a is Zb bydefinition, a reflectance of a pressure K at the reflecting section 61 acan be expressed by the following equation:K=(Zb−Za)/(Za+Zb)  (12)

Note that an acoustic impedance value Z is obtained by the followingequation:Z=√(M×C)  (13)

M and C herein are effective values of the inertance M and the acousticcapacitance C, respectively.

Note that it is only a high frequency vibration that can be reflectedwith this construction. A guide value of the frequency lower limit hasto be a frequency, wavelengths ½-fold or more the a wavelengthcorresponding to which can reside in a region of the pressure absorbingsection 60 when waves propagate in the pressure absorbing section. Inother words, among frequencies when waves propagate in the pressureabsorbing section 60, no reflection occurs of waves with wavelengths oftwo-fold or more the length (that is Lb) propagating a pressure throughthe pressure absorbing section 60 and reflection occurs on waves withwavelengths shorter than that.

That is, a component with frequencies of a prescribed frequency orhigher becomes hard to propagate ahead of the pressure absorbingsection, a flow of a liquid ahead of this portion can be a smooth flowwithout pulsation. As a result, even if there is a complex flow channelshape such as a sharp bend or a connecting section with an external flowchannel or a indefinite factor such as mixing-in of air bubbles,stabilization of fluid transferring characteristic can be effectivelyrealized without producing no reflection of waves hard to be controlledbecause of the shape or the factor.

There is a case where a reflected wave reflected at the pressureabsorbing section 60 returns to the second opening section 24 of themicropump 20 to thereby affect an influence on a characteristic of themicropump 20. Generally, the influence results in deterioration incharacteristic in more of cases. By performing a design taking intoconsideration a position of a wave front, however, a reflected wave canbe intentionally used to the contrary to enable enhancement ofefficiency. Especially, this effect is greatly exerted in the micropump10 of the type shown in FIGS. 1 and 2.

That is, since in the micropump 10 of the above type, no change in flowchannel resistance value in the second opening section 24 is requiredeven if a pressure changes, a change in pressure across the secondopening section 24 is desired to be the lowest possible level.Therefore, a reflected wave is used to cause the reflected wave having aphase difference from a pressure vibrational cycle wave form tointerfere with the original wave in the second opening section 24 tothereby suppress fluctuation in pressure in the second opening section24, thus enabling better characteristic to be obtained.

For the purpose, it is preferably required to find a distance La fromthe second opening section 24 to the pressure reflecting section 61 a sothat the distance La becomes the most suitable while avoiding a lengthin the vicinity of a length N (N=1,2, 3, . . . ) times a half wavelengthat which a wave of a driving cycle of the micropump 10 propagates a flowchannel. As the N is larger, however, attenuation of the reflected waveincreases; therefore reduction occurs in an effect of suppressingfluctuations in pressure with the reflected wave. Moreover, if awavelength changes by a slight error in design and external disturbance,a phase of a reflected wave shifts, which could lead to a unexpectedresult different from a target altogether. Therefore, it is preferablethat a distance La from the second opening section 24 to the pressurereflecting section 61 a is set to be shorter than ½ times a wavelengthof a driving cycle of the micropump 10 and furthermore to install thepressure reflecting section 61 a at a position so as to make a phase ofthe reflected wave to be the most suitable.

Note that a length of a half wavelength to a driving cycle Tp of themicropump 10 is given in a similar way to the above equation (11) asfollows:Lh=Tp/√(M×C)  (14)

Therefore, it is preferably required that a position (that is a lengthof La) of the pressure reflecting section 61 a for the Lh is optimized,or Lh for a position of the pressure reflecting section 61 a isoptimized by changing a capacitance C of the pressure propagating flowchannel (a portion of La) or an inertance M.

The, description of a first modification of the second embodiment ispresented below with reference to FIG. 7.

A fluid transferring system of FIG. 7 is installed with pressureabsorbing sections 60, 62 and 64 inserting with a spacing therebetweenat plural positions in one flow channel 34. With such a constructionapplied, propagation of a high frequency component can be effectivelyprevented or suppressed. By installing the plural pressure absorbingsections 60, 62 and 64 in such a way, reflections at respectiveboundaries 61 a, 61 b, 63 a, 63 b, 65 a and 65 b are not required to beso intense as in a case of FIG. 6, therefore, a high frequency componentpropagating ahead of the pressure absorbing section 64 can be suppressedby reducing wave components reflecting back to the second openingsection 24.

A pressure absorbing section may be of a construction other than FIGS. 6and 7 and it is preferably required that there is a boundary at which anacoustic impedance Z is discontinuous.

Furthermore, such a reflection phenomenon can also be produced in aportion where straight propagation of a pressure wave is hindered suchas a portion where a flow channel suddenly bends regardless of a valueof an acoustic impedance, such a portion can also used for a similarpurpose.

For example, in a fluid transferring system of FIG. 8, plural bentsections 34 k can be provided in a portion 34 s ahead of the flowchannel 34 to thereby enable part of a high frequency wave to bereflected in the bent sections 34 k.

Then, description will be given of a third embodiment with reference toFIGS. 9 to 16.

A plurality of micropumps such as those in the first and secondembodiments are arranged and the micrpumps are connected into a systemto thereby enable a characteristic as a system to be improved more thanwhen one micropump is single used. In a case where such a way of use isadopted, it is possible that a micropump receives no influence ofpulsation from the other micropumps and to the contrary, by mutuallyusing pulsation of individual micropumps, the combination of micropumpsis of higher performance.

In a fluid transferring system shown in FIG. 9, micropumps 10 a and 10 bconnected to respective liquid chambers 30 a and 30 b are arranged toconstruct parallel lines and to increase a flow rate as a system. Atthis time, in order to prevent occurrence of unexpected inconvenience atmerging section 34 c by influences of mutual pulsation of the micropumps10 a and 10 b and a change in characteristic of a flow in a flow channel36 after the merging, pressure absorbing sections 60 a and 60 b arerespectively installed at some mid points in the flow channels 34 a and34 b connected to the micropumps 10 a and 10 b.

Fluid transferring systems of FIGS. 10 and 11 have a plurality ofmicropumps 10 c and 10 d connected in series between the liquid chamber30 and the flow channel 38 to thereby, increase a generated pressure asa system. At this time, it is predicted that an interference of pressurewaves occurs between the micropumps 10 c and 10 d by influences ofmutual pulsation of the micropumps 10 c and 10 d to thereby, disable adesired characteristic to be obtained. In order to prevent this, in thefluid transferring system of FIG. 10, a pressure absorbing section 60 isinstalled in the flow channel 34 connecting the chambers of therespective micropumps 10 c and 10 d therebetween. In the fluidtransferring system of FIG. 11, only the pressure absorbing section 60is installed between the micropumps 10 c and 10 d without a flowchannel. This method can be used to all micropumps of any types havingpulsation, not limited to the micropump of the type of FIG. 1.

In a case where plural micropumps are connected in series, there is amethod in which pressure waves of the respective micropumps are used byeach other to raise characteristics thereof in addition to alleviatepulsating pressures. The example of the method will be shown below.

In a fluid transferring system of FIG. 12, chambers of plural micropumps40 a, 40 b and 40 c are connected in series between flow channels 31 and35 (no problem occurs if the chambers are connected through flowchannels) and phase differences are imparted between adjacent micropumps40 a, 40 b and 40 c (or shifting timings of respective drivingvoltages), in which situation, the micropumps are driven.

In FIG. 13( a), there is shown a fluid transferring system of aconstruction in which two micropumps of the type shown in FIGS. 1 and 2are installed in series with each other. In this system, to be concrete,chambers 20 s and 20 t of two micropumps 10 s and 10 t are connected bya common first opening section 22 x therebetween and the other sides ofthe chambers 20 s and 20 t are connected to flow channels 31 and 35through second opening sections 24 s and 24 t. The micropumps 10 s and10 t are properly driven so that a behavior of an actuator causes themicropumps 10 s and 10 t to have a phase difference therebetween (or apolarity, positive or negative in a deformation direction is reversed tonegative or positive). For instance, FIG. 13( b) is examples of drivingvoltage waveforms 80 and 82 applied to the respective actuators (notshown in FIG. 13( a)) of the micropumps 10 s and 10 t. Driving voltagewaveforms 80 and 82 are synchronized between a steep rise 80 a and asteep fall 82 a and between a mild fall 80 b and mild rise 82 b andphases between waveforms of both micropumps 10 a and 10 t are shifted by180 degrees.

FIG. 14( a) is a fluid transferring system with a fifth modification ofthe third embodiment in which chambers 20 s and 20 t of micropumps 10 sand 10 t of the type of FIG. 1 are connected by a common second openingsection 24 x, and first opening section 22 s and 22 t on the other sidesof the chambers 20 s and 20 t are connected to flow channels not shownthrough pressure absorbing section 60 s and 60 t. In this case, thepressure absorbing section 60 s and 60 t are desirably installed fromthe viewpoint of a sable characteristic. FIG. 14( b) are examples ofdriving voltage waveforms 84 and 86 applied to actuators (not shown inFIG. 14( a)) of the micropumps 10 s and 10 t. The actuators of themicropumps 10 s and 10 t have respective different rise times (lengthsof 84 a and 86 a) and respective different fall times (lengths of 84 band 86 b) and in the rises and falls of the waveforms, when adisplacement velocity of one of the actuators is the fastest, directionsof displacement of both actuators coincide with each other.

In a fluid transferring system of FIG. 15, which is a sixth modificationof the third embodiment, plural micropumps 40 s and 40 t are connectedin series between flow channels 31 and 35 through a flow channel 33,which is a connection section. By setting a length L₀ of the flowchannel 33 to a proper value, pulsations produced by the micropumps 40 sand 40 t can be used by each others with respect of a wavelength of apressure compressional wave propagating through the flow channel 33.

As described above, it is preferably required that the length L₀ of theflow channel 33 may be set so that a pressure compressional wavepropagating from one micropump to the other pump and a reflected wavecancel each other avoiding values in the vicinity of N (N=1, 2, . . . )times a half wavelength of the pressure compressional wave. When alength L₀ of a flow channel 33 is ½-fold or less the wavelength of apressure compressional wave, attenuation of a reflected wave is small;therefore not only does a canceling effect increase, but a target resultcan also be achieved even if design error, manufacturing error, externaldisturbance or the like occurs.

If the flow channel 33 is excessively short, however, the effect cannotbe attained and what's worse a possibility arises that an adverseinfluence is exerted. In a sine wave, which is the most popular pressurecompressional wave, a length from a position of a peaked pressure to aposition where a pressure is zero corresponds to a length ¼ times thewavelength and in a case of the length or less, so much of the effectcannot be expected and to the contrary, an adverse effect is likely tobe exerted. Therefore, a length L₀ of the flow channel 33 is desirablyequal to or more than ¼ times the wavelength of a vibration with adriving frequency.

With any combination of the above various contrivances applied, a fluidtransferring system with higher performance can be constructed.

For example, a fluid transferring system of FIG. 16 (seventhmodification of third embodiment) is constructed of three parallel lineseach including a first micropump, a first flow channel containing afirst pressure absorbing section, a second micropump and a second flowchannel connected in the order between a liquid reservoir 30 x and asecond pressure absorbing section 60 x, wherein the three firstmicropumps are indicated with 10 u, 10 v and 10 w; the three first flowchannels with 34 u, 34 v and 34 w; the three pressure absorbing sectionswith 60 u, 60 v and 60 w; the three second micropumps with 10 x, 10 yand 10 z; and the three second flow channels with 34 x, 34 v and 34 w.By merging the lines in each of which constituents are connected inseries but the whole of which are connected in parallel, a flow rate anda generated pressure of the flow channel 36 after the merging can beincreased.

As described above, a fluid transferring system can prevent itscharacteristic from deteriorating by installing a pressure absorbingsection, a reflecting section and others therein.

Then, description will be given of the first modification example of thefirst embodiment described in FIG. 3 in a more detailed manner. Sincethe micropump 10 shown in FIG. 1 realizes a pumping action by using adifference in flow channel characteristic between the two openingsections 22 and 24, a pump having a larger difference in flow channelcharacteristic obtains a larger flow rate with a better efficiency. Thatis, the one opening section 22 is better in efficiency with the largestpossible differential pressure dependency while the other openingsection 24 is better with a smaller differential pressure dependency.

Therefore, in the first modification of the first embodiment, the fluidtransferring system is constructed using the opening section 24 small indifferential pressure dependency as an opening section group (or a groupof sub-opening sections). That is, the opening section group 24 includesthe two sub-opening sections 24 a and 24 b provided in parallel to eachother and the flow channel 34 communicates with the chamber 20 throughthe two opening sections 24 a and 24 b.

The micropump of this modification is also driven by an actuator of amonomorphic structure including the piezoelectric element 16 and thethin plate 14. A voltage of a waveform shown in FIG. 20( a) or FIG. 21(a) is applied to the piezoelectric element 34 by the driving circuit 18to thereby bend and deform the actuator and to increase or decrease avolume of the chamber 11.

An effective sectional area of the opening section 22 is smaller than aneffective sectional area of the reservoir 30. Furthermore, effectivesectional areas of the respective opening sections 24 a and 24 b aresmaller than that of the flow channel 34. A change ratio as a whole inflow channel resistance of the opening section group 24 when a pressurein the chamber 20 is raised or lowered is set to a value smaller thanthat of the opening section 22.

That is, while the opening section group 24 is constituted of the twoopening sections 24 a and 24 b, the opening sections 24 a and 24 b areequal in aspects of a length, a sectional shape and an effectivesectional area to each other. Therefore, to simply consider theconstruction, a flow channel resistance is halved compared to the caseone of the opening sections 24 a and 24 b is used.

By comparison with the micropump 10 of the first embodiment, the firstmodification of the first embodiment can be regarded as a micropump of aconstruction in which the two opening sections 24 a and 24 b each withthe same sectional shape as the single opening section 24 are providedinstead of the single opening section 24 and a length of the openingsections 24 a and 24 b are increased (to, for example, the order of avalue twice) so as not to reduce a flow channel resistance as a whole.

Therefore, as shown in FIG. 22( a), the opening section 22 shows a lowflow channel resistance when a difference between pressures at both endsis close to zero while showing a higher flow channel resistance when alarger difference between pressures. That is, the differential pressuredependency of the flow channel resistance is high. The opening sectiongroup 24, as shown in FIG. 22( b), shows a flow resistance higher thanin the case of the opening section 22 when the differential pressure isclose to zero, but the flow channel resistance has nearly nodifferential pressure dependency, no much change in flow channelresistance occurs even when the differential pressure is large and theflow channel resistance is smaller than that in the opening section 22when the differential pressure is large.

Such a flow channel resistance characteristic can be attained byadopting a condition that a fluid, that is a liquid, flowing in a flowchannel assumes a laminar flow or a turbulent flow according to adifferential pressure, or alternatively, assumes a laminar flow at alltimes regardless of a differential pressure. To be concrete, thecondition can be realized in the construction in which in the formercase, for example, the opening section 22 is a short orifice in a flowchannel length and in the latter case, the opening sections 24 a and 24b are long nozzles in a flow channel length.

By using such flow channel resistance characteristics of the openingsection 22 and the opening section group 24 not only to generate apressure in the chamber 20 but also to control a change ratio in thepressure, a pumping action can be realized that more of a fluid isdischarged into or taken in from the opening section 22 or the openingsection group 24, whichever is lower in flow channel resistance, in adischarge step and an intake step.

That is, as a pressure in the chamber 20 is raised with the largepressure change rate (or the fast change in pressure), the differentialpressure increases to cause a flow channel resistance of the openingsections 22 to become larger than that of the opening section group 24and to thereby discharge almost all the fluid in the chamber 20 throughthe opening section group 24 (discharge step). As pressure in thechamber 20 is lowered with the small pressure change rate (or the slowchange in pressure), the differential pressure is maintained small tocause a flow channel resistance of the opening section 22 to becomesmaller than that of the opening section group 24 and to thereby causemore of a fluid to be taken into the chamber 20 from the opening section22 (intake step).

Contrary to this, as a pressure in the chamber 20 raised with smallpressure change rate, the differential pressure is maintained small tocause a flow channel resistance of the opening section 22 to be smallerthan that of the flow channel section group 24 to thereby cause more ofa fluid in the chamber 20 to be discharged from the opening section 22(discharge step). As a pressure in the chamber 20 lowered with largepressure change rate, the differential pressure is increased, to cause aflow channel resistance of the opening section 22 to become larger thanthat of the opening section group 24 to thereby cause more of a fluid tobe taken into the chamber 20 from the opening section group 24 (intakestep).

Such a pressure control of the chamber 20 is realized by controlling adriving voltage supplied to the piezoelectric element 16 to furtheradjust a deformation amount of a diaphragm and a timing. For example, byapplying a driving voltage of the waveform shown in FIG. 20( a) to thepiezoelectric element 16, a fluid is discharged into the flow channel 34side while by applying a driving voltage of the waveform shown in FIG.21( a), a fluid is discharged into the reservoir 30 side.

In the FIGS. 20( a) and 20(b), and FIGS. 21( a) and 21(b), the maximumvoltage e1 applied to the piezoelectric element 16 is on the order inthe range of from several volts to tens of volts or on the order of 100volts at the highest. Times T1 and T7 are on the order of 20 μs, timesT2 and T6 is in the range from 0 to several μs and times T3 and T5 areon the order of 60 μs. Times T4 and T8 may be 0. A frequency of adriving voltage is on the order of 11 kHz. In the flow channel 34, forexample, flow rates as shown in FIG. 20( b) and FIG. 21( b) are obtainedaccording to the driving voltages shown in FIG. 20( a) and FIG. 21( a).Note that flow rate curves in FIG. 20( b) and FIG. 21( b) are thoseshown as a model of flow rates obtained by a pumping action and aninertia vibration of a fluid is actually superimposed thereon.Accordingly, these flow rate curves shown in the figures on whichvibrational components are superimposed give flow rates that would beactually obtained.

Focusing again attention on FIG. 22( b), a two-dot chain line shown inthe same figure is flow channel resistance characteristics of theopening section 24 in the construction of FIG. 1. By comparison with aflow resistance characteristic in the construction of the firstembodiment, the opening section group 24 of this modification isunderstood to be small in pressure dependency of flow channelresistance. That is, by giving consideration to this together with FIG.22( a), in a case where the differential pressure is in the range offrom −100 kPa to +100 kPa, it is understood that a flow channelresistance of the opening section group 24 is larger when a value (inthe absolute value) of the differential pressure is small while a flowchannel resistance of the opening section group 22 is larger when avalue of the differential pressure is larger. In addition, a differencein flow channel resistance is larger in any case as compared to a casewhere the opening section 24 in the construction of FIG. 1.

Therefore, according to the micropump 1 of this modification, a flowrate larger with a better efficiency (a flow rate efficiency) than inthe case of the first embodiment by a change in difference in flowchannel resistance.

Then, description will be given of a reason for reduction in pressuredependency due to the use of the plurality of the opening sections,which is not obtainable from a single opening section. The “flow channelresistance” described above, corresponds to a pressure loss coefficient.A flow channel resistance R [N·s/m⁵] is given by the following formulaif a volume (a flow rate) flowing in a unit time is Q, a pressure losscaused by a flow of a fluid is ΔP by definition:R=ΔP/Q  (1)

Herein, N is a force (in units of Newton) and s is a time (in units ofsecond).

Note that the terms “a flow channel resistance of an opening section” or“a flow channel resistance of an opening section group” are a value of aflow channel resistance when a fluid flows forward or backward between aflow channel and a chamber between which the opening section or theopening section group communicates and includes a flow channelresistance caused by a flow in the vicinity of an inlet/outlet of theopening section or the opening section group.

Therefore, in cases where a portion in which a flow velocity is fasterthan a peripheral region thereof or where a turbulent flow occurs in thevicinity of the inlet/outlet, flow channel resistance of the portionsshould be considered as components of the “flow channel resistance ofthe opening section.” Note that in the following description, since anopening section and an opening section group are a kind of a flowchannel, those are also described as “flow channels.”

As described above, generally speaking, a state in which no changeoccurs in flow channel resistance even if a change occurs indifferential pressure between the inlet and outlet of a flow channel (ora flow velocity in the flow channel) is a characteristic in a case wherea laminar flow is sufficiently grown.

Contrary to this, a state in which an increase in flow channelresistance occurs with an increase in differential pressure between theinlet and outlet of a flow channel is a characteristic of a turbulentflow. To be more exact, it can be said a characteristic in a case whereformation of a laminar flow is insufficient.

In general, while a fluid shows a behavior of a laminar flow in theinterior of a thin, long flow channel, a flow channel resistanceincludes components from behaviors of a turbulent flow (or a flow thatis not grown enough to be a laminar flow) in the vicinity of each of theinlet and outlet of the flow channel.

Herein, in a case where consideration is given to a thin, long openingsection with a length, a value Ra of a flow channel resistance is thesum of an invariable component R1 independently of the differentialpressure and a component R2 increasing with the differential pressure,that is expressed by the following formula:Ra=R1+R2  (2)

R1 is a component proportional to a flow channel length L and R2 is acharacteristic associated with both ends and a component independent ofthe flow channel length L.

As shown in FIG. 23, in the opening sections 24 a and 24 b, a componentcaused by a portion with a uniform sectional shape is R1 and a componentcaused by both end portions works is R2.

On the other hand, a value Rb of a flow channel resistance of an openingsection N times a length of the opening section is given by thefollowing formula:Rb=N×R1+R2  (3)

That is, only the component R1 which is proportional to a flow channellength L grows to be N times larger. The meaning of the growth of thecomponent R1 is that only the component R1 invariable independently ofthe differential pressure is N times larger and no change arises in thecomponent R2 increasing with the differential pressure.

Plural flow channels in number of N are arranged in parallel to eachother, a value Rc as a whole of flow channel resistance is given by thefollowing formula, which is deduced by dividing the above formula (3) byN:Rc=R1+R2/N  (4)

As can be understood by comparison between the formulae (2) and (4), theinvariable components R1 independently of the differential pressure areequal therebetween but the component R2 increasing with the differentialpressure, in a case where N flow channels are arranged in parallel toeach other, is 1/N times that in the case of a single flow channel,which decreases with an increased N number of flow channel connected inparallel to each other.

For example, in the above micropump 1, a flow channel resistance ishalved and in the example shown in FIG. 24, a flow channel resistance isto be one-third.

As a result, with an increased number N of flow channels connected inparallel to each other, a change ratio in flow channel resistancedecreases when the differential pressure changes, while improvementoccurs on flow rate characteristic as a pump since a difference inpressure dependency increases compared with the other flow channels.

In such a way, with an increased number N, an efficiency becomes betterin principle, while no differential pressure arises if the number Nbecomes a certain level or larger, so the numbers of N are determinedconsidering a level at which an opening section is fabricated with ease.

Then, there are shown concrete examples of dimensions of sections.

The opening section 22 is on the order of 25 μm in width and on theorder of 25 μm in length. The opening sections 24 a and 24 b are on theorder of 36 μm in width and on the order of 400 μm in length. A depth ofthe opening section 22 and the opening sections 24 a and 24 b are all onthe order of 25 μm and all have a uniform section shape (a section of aflow channel) in the length direction thereof (a direction of a flow ofa fluid).

Note that, on this occasion, a value of L/S, that is [a flow channellength/a sectional area] (in units of μm⁻¹) is 0.04 in the openingsection 22 while being a value as large as 0.44 in the opening sections24 a and 24 b both.

While a letter L used here is a length of a flow channel of an openingsection, a case arises where which length is a proper one is not clearaccording to shapes of both ends of the opening section. In this case,experiments have only to be conducted concerning opening sections withvarious kinds of shapes to find equivalent flow channel lengths of theactual opening sections based on results of the experiments and to usethe equivalent flow channel lengths as effective flow channel lengths.This is also true for a sectional area S.

Here, for a reference, comparison is performed with a construction inwhich a second opening section is one narrow small flow channel. In thiscase, if it is assumed that a width of a second opening section is onthe order of 36 μm and a length is on the order of 180 μm, a value of aflow channel resistance is altered in the range of 7.6 to 15.9(×10¹²N·s/m⁵) under a differential pressure in the range 1 kPa to 100kPa.

In contrast to this, a change in flow channel resistance is in the rangeof from 7.6 to 11.1(×10¹²N·s/m⁵) in a case where the opening sectiongroup 24 according to the modification described above; thereby enablingdecrease in a range of a change to a half or less.

Note that the reservoir 30 and the flow channel 34 may also be a flowchannel in a literal sense in order that a fluid is caused to flowthrough and guided to a prescribed position and a chamber to conduct areaction with a fluid, or alternatively, a something like a reservoir tostore a fluid. In the following description of the presentspecification, both are also collectively referred to “a flow channel.”

As described partly above, the three opening sections 24 a, 24 b and 24c may be provided as the opening section group 24 as shown in FIG. 24.In this case, sectional areas of the opening sections 24 a, 24 b and 24c may be handled as a case of a single opening section with a lengththree times a length of each opening section 24 a, 24 b or 24 c.Furthermore, flow channels each constituting an opening section groupincluding plural opening sections can be merged therebetween into oneflow channel having opening section groups each including plural openingsections.

Then, description will be given below of another construction of thefirst modification as a third modification of the first embodiment. FIG.25 is a model plan view showing a construction of a fluid transferringsystem of a third modification relating to the first embodiment. In thismodification, constituents with the same functions as those of the firstmodification of the first embodiment are attached with the same symbolsand any of descriptions of the constituents is omitted forsimplification.

In this modification, a micropump 10B has a third opening section 26additionally and the opening section 26 is connected to the flow channel35. A flow channel resistance characteristic of the opening section 26can be set in various ways. For example, it may be designed so as tohave the same dimensional shape as the single opening section 24 a tothereby adopt the same flow resistance characteristic as the openingsection 24 a. Furthermore, it may be designed so as to have a sectionalshape larger than the single opening section 24 a but the same length tothereby give a flow resistance characteristic analogous to the flowchannel resistance characteristic shown with a two-dot chain line inFIG. 22( b). Moreover, it may be designed so as to have the samedimensional shape as the opening section 22 to thereby give the sameflow channel resistance characteristic as the opening section 22.

In the micropump 10B of this modification as well, a good flow rateefficiency can be achieved because of a difference in flow resistancecharacteristic between the opening section group 13 and the openingsection 12.

In addition thereto, a working is enabled that a fluid is dischargedinto the flow channel 35 or is taken in from the flow channel 35according to a flow channel resistance characteristic of the thirdopening section 26. On this occasion, a working is enabled that one ofdischarging and intake is conducted and in addition, ratios in flow rateratio therebetween are controlled according to flow resistancecharacteristics of the opening section 22, the opening section group 24and the opening section 26, respectively. In this case, the micropump10B can be used as a mixer of fluids or a flow divider thereof.

Furthermore, a construction may be adopted in which an opening sectiongroup including two opening sections arranged in parallel to each otherreplaces the opening section 26. Especially in a case where the openingsection groups 24 and 26 are both small in change ratio in flow channelresistance between pressures, the flow channels 34 and 35 can securestable flow rate ratios (discharge ratios or intake ratios) thereof atall times even when a driving condition fluctuates or a driving voltageis altered. Accordingly, a merit is exerted that dividing of a flow ormixing of flows both at a stable ratio can be assured. Four or moreopening sections and flow channels may be connected to the chamber 20.

In the second modification described above, the opening section 22larger in differential pressure dependency may also be an openingsection group including plural opening sections.

While in the embodiments and modifications thereof, plural flow channelsare connected to the single chamber 20, all or part of the plural flowchannels may be used as a flow channel in a circulating system.Furthermore, flow channels thereof may be merged at downstream positionremote from the chamber 20. In that case as well, the merged flowchannels is handled not as a single flow channel, but may be handled asflow channels as originally connected individually to the chamber 20.

While in the first, second and second modifications relating to thefirst embodiment, there is shown examples in which the micropumps 10 and10B are fabricated using silicon substrates, the micropumps 10 and 10Bmay also be micro-fabricated from a material such as a resin, glass, ametal, a ceramic or the like. The diaphragm 15 is formed not by halfetching but by laminating a thin plate separately prepared. In thelatter case, any material may be used but a caution is required to betaken since a possibility exists that no sufficient displacementcharacteristic can be attained if the material is extremely softer thana piezoelectric element. Furthermore, while a depth of the chamber 20 isset to be the same as that of an opening section, no necessity arisesfor being the same but a depth of the chamber 20 may be deeper orshallower than that of the opening section. A deformation of thepiezoelectric element 16, serving as an actuator increasing ordecreasing a volume of the chamber 20, has no inevitability to be aunimorphic bending deformation, but may also be, for example, a verticalvibration, a lateral vibration, a shear deformation oscillation or thelike. As the actuator, no specific limitation is placed on thepiezoelectric element 16, but any of materials such as an electrostaticactuator, an electromagnetic actuator or a shape-memory alloy can beused as far as the materials can increase or decrease a volume of thechamber 20. Furthermore, the actuator is not integrated with themicropump 10 or 10B into one piece, but may be separable as a differentidentity.

Though a shape of an opening section is said to be uniform in flowchannel section, no necessity arises for a perfectly uniform section. Inother wards, a uniform sectional shape is not necessary required. Forexample, there are allowed the presence of projections and depressionsor tapers at some level on the inner surface. A practical sectional areaor an effective sectional area S in each of the cases can be obtainedbased on experimental values or calculated values. A widening portionwith some extent area or a smoothly widening edge-rounded portion can beallowed in the vicinity of the inlet/outlet of an opening section,especially in an opening section on the discharge (outlet) side.Moreover, in an opening section in the side serving as the intake port(inlet), no function changes to a great extent even without a uniformsectional shape. To sum up, flow channel resistance characteristics fora pressure change of opening sections interposed in respective flowchannels are different from each other and it is preferably requiredthat a flow channel resistance characteristic of an opening section of aflow channel in which a pumping action is desired to obtain, isdifferent as largely as possible from the others. A fluid that can beapplicable may be a liquid, a fluid, a gas or the like.

While in the first, second and third modifications of the firstembodiment described above, a driving voltage of an approximatetriangular waveform is applied to the piezoelectric element 34, it ispossible to use a driving voltage of one of various other kinds ofwaveforms. Moreover, a shape of a plan view of the micropump 1 or 10Bcan assume a square, a rectangle, a polygon, a circle, an ellipse andvarious other kinds of shapes. In addition thereto, the whole or partsof a micropump can be properly altered according to the spirit and scopeof the present invention in aspects of a structure, a shape, adimension, the number, a material and others.

For example, the present invention is not limited to a case where twoflow channels communicating with a chamber of a micropump, but a casemay be adopted where three or more independent flow channels communicatewith a micropump as described in connection with the third modificationof the first embodiment. In this regard, a fourth embodiment of thepresent invention will be described below.

FIG. 26 and FIG. 27 are a schematic plan view and a schematic frontsectional view showing a construction of a micro-fluid transferringsystem of a fourth embodiment of the present invention, FIG. 28 is agraph showing a flow channel resistance characteristic of each openingsection, FIG. 29 and FIG. 30 are graphs showing example waveforms of adriving voltage of a piezoelectric element and FIG. 31 is a graphshowing a way of change in volume of the chamber 20 according to adriving voltage. Note that FIG. 27 shows a section taken in planepassing through the centers of a reservoir 30, an opening section 22, achamber 20, an opening section 24 and a flow channel 34 of FIG. 26.

The micro-fluid transferring system, as shown in FIG. 26 and FIG. 27,includes: a chamber 20, which is a pump room; first, second and thirdflow channels 22, 23 and 24, whose number is 3 in total, connected tothe chamber 20; and first, second and third opening sections 22, 24 and26 provided to flow channels 30, 34 and 35 in order to reduce flowchannel sections thereof.

The micro-fluid transferring system, as well shown in FIG. 27, isfabricated in a procedure in which a silicon substrate 12 is used, thefollowing grooves and recesses are formed in a photolithographic step:such as the chamber 20, the opening sections 22, 24 and 26 and flowchannels 30, 34 and 35 and others and a glass substrate 19 serving as abase plate is adhered to the lower surface of the silicon substrate 12.On this occasion, a recess serving as the chamber 20 in the siliconsubstrate 12 is obtained by half-etching the silicon substrate 12 so asnot to be etched therethrough and the rest portion of the siliconsubstrate 12 is used as a diaphragm 15. A piezoelectric element 16 isadhered onto the diaphragm 16.

While the micro-fluid transferring system can be fabricated in such away, the system can also be fabricated using a prior art publicly knownmethod, other methods or other materials.

As the piezoelectric element 16, similar to the above examples, forexample a PZT ceramics thin plate is used. Two electrodes for drivingthe piezoelectric element 16 is wire-led out onto surfaces at both sidesof the piezoelectric element 16 and connected to a flexible cable or thelike to be further connected to a driving circuit DR by the flexiblecable.

The piezoelectric element 16 is applied with a voltage of a waveformshown in FIG. 29( a) or FIG. 30( a) to thereby cause the diaphragm 15,which is a silicon thin film, and the piezoelectric element 16 to besubjected to a bending deformation in the unimorphic mode and toincrease or decrease a volume of the chamber 20.

For example, when a driving voltage of a triangular waveform is used forsimplicity as shown in FIG. 31( a), a volume of the chamber 20, as shownin FIG. 31( b), alters according to the waveform of the driving voltage.

Now, in this embodiment, the first, second and third opening sections22, 24 and 26 are set so that change ratios in flow channel resistancethereof are different from each other when a pressure in the chamber 20is raised or lowered. The change ratios are set so as to decrease in theorder of the first, second and third opening sections, that is, so thatthe first opening section 22 shows the largest change ratio, the secondsection 24 shows the second largest change ratio and the third openingsection 26 shows the lowest change ratio.

That is, the first opening section 22, as shown in FIG. 28, shows a lowflow channel resistance when a difference in pressure between both endsthereof is close to zero, but with an increased differential pressure, aflow channel resistance becomes larger. In other words, the firstopening section 22 has a large differential pressure dependency. Thethird opening section 26 shows a large channel resistance when adifferential pressure is close to zero, but has nearly no differentialpressure dependency and even if a differential pressure becomes larger,a flow channel resistance increases to a value of the order a littlelarger than before. A differential pressure dependency of a flow channelresistance of the second opening section 24 show an intermediate valuebetween those of the first opening section 22 and the third openingsection 26.

Such flow channel resistance characteristics can be selected accordingto whether or not a fluid, for example a liquid, flowing in a flowchannel assumes a laminar flow or a turbulent flow depending on a valueof a differential pressure, or alternatively, selected so as to assume alaminar flow regardless of a value of a differential pressure. That is,shapes of the first, second and third opening sections 22, 24 and 26 maybe designed so that a laminar flow grows to a more sufficient levelwhile suppressing occurrence of a turbulent flow to a lower level in theorder of the first, second and third opening sections 22, 24 and 26.

To be concrete, for example, the first opening section 22 is designed asan orifice with a short flow channel length, the third opening section26 is designed as a nozzle with a long flow channel length and thesecond opening section 24 is designed to have an intermediate lengththerebetween.

A construction is recommended when viewed from another angle in whichthe opening sections 22, 24 and 26 are designed so as to be uniform inflow channel section, a ratio of a flow channel length to a sectionalarea is set so as to increase in the order of the first, second andthird opening sections 22, 24 and 26, and dimensional shapes thereofhave regions in which flow channel resistance values of respectiveopening sections are inverted in magnitude between each other in anactually used range of differential pressures.

Accordingly, focusing attention on the first opening section 22 and thethird opening section 26, as a pressure is increased with a largepressure change ratio (or fast change speed in pressure) of the chamber20, a differential pressure increases to thereby cause a flow channelresistance of the opening section 22 to become larger than a flowchannel resistance of the opening section 26, with the result thatalmost all the fluid in the chamber 20 is discharged from the openingsection 26. As a pressure is reduced with a small pressure change ratio(or slow change speed in pressure) of the chamber, a differentialpressure is maintained at a small value to cause a flow channelresistance of the opening section 22 to be smaller than a flow channelresistance of the opening section 26 and to cause more of a fluid toflow into the chamber 20 from the opening section 22.

Contrary to this, as a pressure is increased with a small pressurechange ratio (or slow change speed in pressure) of the chamber 20, adifferential pressure is maintained at a small value to cause a flowchannel resistance of the opening section 22 to be smaller than a flowchannel resistance of the opening section 26 and to cause more of afluid in the chamber 20 to be discharged from the opening section 22. Asa pressure is reduced with a large pressure change ratio (or fast changespeed in pressure) of the chamber 20, a differential pressure becomeslarger to cause a flow channel resistance of the opening section 22 tobe larger than a flow channel resistance of the opening section 26 andto cause more of a fluid to flow into the chamber 20 from the openingsection 26.

Such a pressure control of the chamber 20 is realized by controlling adriving voltage supplied to the piezoelectric element 16 to furthercontrolling a deformation amount of a diaphragm and a timing. Forexample, by applying a driving voltage of the waveform shown in FIG. 29(a) to the piezoelectric element 16, a fluid is discharged into the flowchannel 35 side while by applying a driving voltage of the waveformshown in FIG. 30( a), a fluid is discharged into the flow channel 30side.

In FIGS. 29( a) and 29(b), and FIGS. 30( a) and 30(b), the maximumvoltage e1 applied to the piezoelectric element 16 is on the order inthe range of from several volts to tens of volts and on the order of 100volts at the highest. Furthermore, taking up one examples associatedwith a time, times T1 and T7 are on the order of 20 μs, times T2 and T6are on the order in the range of from 0 to several μs and times T3 andT5 are on the order of 60 μs. Times T4 and T8 may also be 0. A frequencyof a driving voltage is on the order of 11 kHz. With driving voltagesshown in FIG. 29( a) and FIG. 30( a) applied, for example, flow rates asshown in FIG. 29( b) and FIG. 30( b) are obtained in the flow channel35. Note that flow rate curves in FIG. 29( b) and FIG. 30( b) show flowrates obtained by a pumping action as a model and inertia vibrations areactually superimposed on the flow rate curves. Therefore, actual flowrates are shown by curves obtained by superimposing a vibrationcomponent on the flow rate curves shown in the figures.

However, since the second opening section 24 participates in dischargeand intake, an actual fluid flow is more complex.

Therefore, such flow channel resistance characteristics of the openingsections 22, 24 and 26 are used not only to generate a pressure in thechamber 11, but also to control a change ratio in pressure, and tothereby transport a liquid at a flow rate and in a direction accordingto values of flow channel resistance of the opening sections 22, 24 and26 at that time, thereby enabling plural fluid flows to be merged or afluid flow to be divided into plural fluid flows.

For example, as shown in FIG. 29 and FIG. 30, at least two kinds ofdriving voltage waveforms are prepared and change-over is performedtherebetween. Furthermore, the maximum voltage e1 may be altered withthe same waveform adopted. Furthermore, a waveform and a maximum voltageare arbitrarily altered to enable a fine control of a dischargedirection, a flow rate, a flow rate ratio and the like.

In a case where fluids from plural flow channels are merged in thechamber 20, the chamber can work, for example as a mixer. In a casewhere a fluid is discharged into plural flow channels from the chamber20, the chamber can work as pumps discharging fluids at prescribedratios to the plural flow channels, or alternatively, as a flow divideror a flow channel change-over unit.

The flow channel resistance characteristic curves of the three openingsections 22, 24 and 26, as shown in FIG. 28, are more effectively set ina relation in which the curves intersect with each other in a range ofdifferential pressures in use. This is because values of flow channelresistance between any two flow channels are inverted in a transitionfrom a case where a differential pressure is larger in absolute valuethan the differential pressure as the center at an intersection of thecurves to a case where a differential pressure is smaller in absolutevalue than the differential pressure as the center, or vice versa,thereby enabling achievement of improvement on a flow rate efficiency.While that in such a way, values of flow channel resistance are invertedin magnitude is not necessarily required in order to cause a fundamentalfunction as a micro-fluid system 1 to be fully exerted, it is animportant factor to improve a flow rate efficiency.

Furthermore, in FIG. 28, the three curves do not intersect with eachother at a single point, and, therefore, in a certain differentialpressure range, the large and small order of the flow channelresistances of the three opening sections 22, 24 and 26 is changed. Bysetting changes in flow channel resistance characteristics in a suitableway, various functions described above can be enhanced to respectivehigher levels.

Then, there are shown concrete examples of dimensions of sections.

The opening section 22 is on the order of 25 μm in width and on theorder of 25 μm in length. The opening section 24 is on the order of 30μm in width and on the order of 90 μm in length. The opening section 26is on the order of 36 μm in width and on the order of 180 μm in length.A depth of the opening sections 22, 24 and 26 are all on the order of 25μm and all have a uniform sectional shape (a section of a flow channel)in the length direction of a flow channel (the direction of a flow of afluid).

Note that, on this occasion, a value of L/S, that is [a flow channellength/a sectional area] (in units of μm⁻¹) is 0.04 in the openingsection 22, 0.12 in the opening section 24 and 0.20 on the openingsection 26, that is a value of [a flow channel length/a sectional area]increases in the ascending order of the first opening section 22, thesecond opening section 24 and the third opening section 26.

While a letter L used here is a length of a flow channel of an openingsection, a case arises where which length is a proper one is not clearaccording to shapes of both ends of the opening section. In this case,experiments have only to be conducted concerning opening sections withvarious kinds of shapes to find equivalent flow channel lengths of theactual opening sections based on results of the experiments and to usethe equivalent flow channel lengths as effective flow channel lengths.This is true for a sectional area S.

Note that the flow channels 30, 34 and 35 each may be a flow channel ina literal sense in order that a fluid is caused to flow through andguided to a prescribed position and a chamber to conduct a reaction witha fluid, or alternatively, a something like a reservoir to store afluid. In the following description of the present specification, theyare also collectively referred to “a flowing channel.”

According to a micro-fluid transferring system, a pumping action forplural flow channels 30, 34 and 35 can be performed by a single chamber20 and control can be exerted of a flow rate and a direction ofdischarge from or intake into the flow channels 30, 34 and 35. A singlepiezoelectric element 16 for change in volume of each chamber 20sufficiently works to thereby cause a construction to be simple and acontrol to be easy; thereby enabling a stable liquid transport to beperformed. Flow channel resistance characteristics of the respectiveopening sections 22, 24 and 26 are set in any suitable way to control adriving voltage applied to the piezoelectric element 16 and to therebyenabling plural fluid flows to be merged at prescribed ratios orenabling a fluid flow to be divided into plural fluid flows atprescribed ratios.

While in the above embodiment, a driving voltage of a triangularwaveform or an approximately triangular waveform is applied to thepiezoelectric element 16, various other kinds of waveforms can be used.The bottom line is that a driving waveform may be any with which a speedof oscillation of increase or decrease in volume of the chamber 20 ismade different according to whether it is at a timing of a rise or afall, in which state the absolute value of the speed has only to be ableto change.

Then, description will be given of a micro-fluid transferring systemaccording to the first modification of a fourth embodiment withreference to FIG. 32. Note that in this modification, constituentshaving the same functions as in the fourth embodiment are attached withthe same symbols and any of descriptions thereof is omitted forsimplicity.

In this modification, there is provided an opening section group 24Bincluding two opening sections 24 a and 24 b connected in parallel toeach other in a second flow channel 34 and an opening section group 26Bincluding two opening sections 26 a, 26 b and 26 c connected in parallelto each other in a third flow channel 26.

That is, the two opening sections 24 a and 24 b constitutes the openingsection group 24B and are equal in length, sectional shape and effectivesectional area to each other. Compared with the opening section 24 shownin FIG. 26, a length of each is twice but an effective sectional area ofeach is equal thereto. With such a construction adopted, a flow channelresistance value as a whole of the opening section group 24B isgenerally almost equal to that of the opening section 24 of FIG. 26, buta change ratio in flow channel resistance as a whole of the openingsection group 24B decreases, resulting in small pressure dependency.

The three opening sections 26 a, 26 b and 26 c constitute the openingsection group 26B and are equal in length, sectional shape and effectivesectional area to each other. Compared with the opening section 26 shownin FIG. 26, a length of each is thrice but an effective sectional areaof each is equal thereto. With such a construction adopted, a flowchannel resistance value as a whole of the opening section group 26B isgenerally almost equal to that of the opening section 26 of FIG. 26, buta change ratio in flow channel resistance as a whole of the openingsection group 26B decreases resulting in pressure dependency smallerthan the opening section group 24B.

For example, in a case where plural opening sections are arranged inparallel to each other without any interference with each other, a valueobtained as a reciprocal of the sum of individual reciprocals of flowchannel resistance values of the plural opening sections can be used asa flow channel resistance as a whole of a group of the plural openingsections.

At least one (in this embodiment, all of them) of the opening sections26 a, 26 b and 26 c provided in the third flow channel 26 is larger invalue of [a flow channel length/a sectional area] than the openingsection 22, or any of the opening sections 24 a and 24 b provided in theother flow channels 30 and 34.

Furthermore, at least one (in this embodiment, all of them) of theopening sections 24 a and 24 b provided in the second flow channel 24 islarger in value of [a flow channel length/a sectional area] than any ofthe opening sections 26 a, 26 b and 26 c provided in the flow channel26.

With reduction in section of the flow channels using the opening sectiongroups 24B and 26B each including plural opening sections connected inparallel to each other, a pressure dependency as a whole of each of theopening section groups 24B and 26B can be decreased to thereby increasea difference in pressure dependency from other opening sections oropening section groups; thereby enabling improvement on a flow ratecharacteristic as a pump.

Then, description will be given of a behavior of a fluid in a case wherea micro-fluid transferring system.

The following Tables 1 and 2 show flow channel resistancecharacteristics and flow rates of the respective opening sections 22, 24and 26 in the micro-fluid transferring system 1.

TABLE 1 Differential Pressure Dependency of Each Opening Section (×1012N · S/m5) Differential Pressure 1 kPa 10 kPa 100 kPa Opening Section22 3.2 6.2 15.4 Opening Section 24 5.0 7.2 15.8 Opening Section 26 7.69.0 15.9

TABLE 2 Flow Rate of Each Opening Section Differential Pressure 1 kPa 10kPa 100 kPa Opening Section 22 48.5% 39.2% 34.0% Opening Section 2431.1% 33.8% 33.1% Opening Section 26 20.4% 27.0% 32.9%

The following Table 3 shows a discharge fluid volume in each time of therespective opening sections 22, 24 and 26 in the micro-fluidtransferring system 1, and Table 4 shows the driving conditions of thedriving patterns A thought D in the Table 3.

TABLE 3 Discharge Fluid Volume of Each Opening Section per One CapacityChange (± 100 pl) of Chamber Driving Pattern A B C D Opening Section 229.3 5.2 −9.3 −5.2 Opening Section 24 −2.7 0.7 2.7 −0.7 Opening Section26 −6.6 −5.9 6.6 5.9

TABLE 4 Driving Conditions of Driving Patterns A though D CompressionState Decompression State A  1 kPa  10 kPa B  10 kPa 100 kPa C  10 kPa 1 kPa D 100 kPa  10 kPa

Herein, definition is given so that flow channel resistance values ofthe opening sections 22, 24 and 26 at a pressure in the chamber 20 whena volume thereof is on the decrease are R1 r, R2 r and R3 r,respectively, and volumes of a fluid coming in and going out of the flowchannels 30, 34 and 35 at that time are V1 r, V2 r and V3 r,respectively.

Furthermore, definition is given so that flow channel resistance valuesof the opening sections 22, 24 and 26 at a pressure in the chamber 20when a volume thereof is on the increase are R1 f, R2 f and R3 f,respectively, and volumes of a fluid coming in and going out of the flowchannels 30, 34 and 35 at that time are V1 f, V2 f and V3 f,respectively.

In addition, a change amount in volume of the chamber 20 (a width of theoscillation) is indicated with V0 by definition. At this time, forexample, a volume ΔV1 of a fluid fed out through the first flow channel30 in one cycle of volume increase/decrease oscillations of the chamber20 is expressed approximately by the following formulae (, which wouldbe somewhat modified, actually, because of inertia vibrations addedthereto):ΔV1=V1r−V1fV1r=V0x(1/R1r)/[(1/R1r)+(1/R2r)+(1/R 3 r)]V1f=V0x(1/R1f)/[(1/R1f)+(1/R2f)+(1/R 3 f)]

Likewise, as for the second flow channel 34 and the third low channel35, a volume of a fluid fed out through the second flow channel 34 orthe third flow channel 35 in one cycle of volume increase/decreaseoscillations of the chamber 20 can be calculated.

Herein, in a case where flow channel resistance characteristics of theopening sections are as shown in Table 1, volumes of a fluid fed outthrough the respective flow channels in one cycle of volumeincrease/decrease oscillations of the chamber 11 are as shown in Table 3using the above formulae.

Note that in the Table 3, a number with a plus sign expresses adischarge direction and a number with a minus sign expresses an intakedirection. As is clear from the Table 3, flow ratios in the openingsections and a direction of a fluid can be changed over differently byaltering a driving pattern of the chamber 20.

Control of a pressure accompanying increase/decrease in volume of thechamber 20, for example, with a fine adjustment of a rise time, a falltime or the like of a driving voltage waveform also enables a subtleadjustment of a flow rate and a flow ratio.

In the above embodiment, while the number of flow channels is three, butfour or more may be adopted. Any of flow channels may have an openingsection group including plural opening sections. Furthermore, an openingsection group provided in a flow channel may be constituted of four ormore opening sections.

In the above embodiment, the flow channels 30, 34 and 35 may also beones in a circulation system. A construction may be adopted in which theflow channels 30, 34 and 35 are merged at a position remote from thechamber 20. In that case as well, the flow channels is unnecessary behandled as a single flow channel, but may be handled as individual flowchannels connected to the chamber 20.

While in the above fourth embodiment and the modification thereof, thereis shown an example in which a micro-fluid system is fabricated using asilicon substrate, the system may be micro-fabricated using a materialsuch as a resin, glass, a metal, a ceramic or the like. The diaphragm isunnecessary to be formed by half etching, but may be formed bylaminating a thin plate prepared separately. In the latter case, anymaterial may be adopted, but a caution should be taken because of apossibility that no sufficient displacement characteristic cannot beobtained in a case where the material is extremely softer than apiezoelectric element.

While in the above fourth embodiment and the modification thereof, adepth of the chamber 20 is the same as an opening section, no necessityexists for being the same but a depth of the chamber 20 may be eitherdeeper or shallower than the opening section. A deformation of thepiezoelectric element 16 serving as an actuator to increase/decrease avolume of the chamber 20 is of no inevitability of unimorph bendingdeformation but may be caused by a vertical vibration, a lateralvibration, a shear deformation oscillation or the like. As the actuator,no specific limitation is placed on the piezoelectric element 16, butany of members such as an electrostatic actuator, an electromagneticactuator, a shape-memory alloy or the like can be used as far as themembers can increase or decrease a volume of the chamber 20.Furthermore, the actuator is not integrated with the micro-fluidtransferring system into one piece, but may be separable as a differentidentity.

Though as to a shape of an opening section, a flow channel thereof issaid to be uniform in section, no necessity arises for a perfectuniformity in section. In other words, a uniform sectional shape is notnecessary required. For example, there are allowed the presence ofprojections and depressions or tapers at some level on the innersurface. A practical sectional area or an effective sectional area ineach of such cases can be obtained based on experimental values orcalculated values. A widening portion with some extent area or asmoothly widening edge-rounded portion can be allowed in the vicinity ofthe inlet/outlet of an opening section, especially at an opening sectionon the discharge (outlet) side. Moreover, in an opening section in theside serving as the intake port (inlet), no function changes to a greatextent even without a uniform sectional shape. A fluid that isapplicable may be a liquid, a fluidized mass, a gas or the like.

Note that the present invention is not limited to the above embodimentsand their modifications, but can be implemented in various otherembodiments.

For example, the present invention is not limited to a case where twoflow channels communicating with a chamber of a micropump, but a casemay be adopted where three or more independent flow channels communicatewith a micropump as described in connection with the second modificationof the first embodiment. Furthermore, a case is also adopted where flowchannels connected to the chamber of a micropump are further connectedto each other to thereby construct a liquid circulating system.

As another examples, FIGS. 33( a) through 33(c) are another structuresof fluid transferring systems to which the present invention isapplicable. FIG. 33( a) is a bottom view of a fluid transferring system.In this example, three discrete fluid transferring portions are providedin a single cell. The single cell mainly comprises, like as the firstembodiment, a base plate 12 and a flat thin plate 14 bonded together.Formed on the upper surface of the base plate 12 are three sets ofrecesses: each set comprises, from left side in this order, recesses fora liquid reservoir 30, a first opening section 22, a chamber 20, asecond opening section 24, and a flow channel 34. On the upper surfaceof thin plate 14, a piezoelectric element (not shown) is fixed at aposition corresponding to the chamber 20 to form an actuator. Thechamber 20, and first and second opening sections 22 and 24 constitute amicropump like as the above mentioned embodiments. At a left edge of theliquid reservoir 30 and right edge of the flow channel 34, respectivelyformed are through holes 100 and 102 that allow each fluid transferringportion to be fluidically connected to neighboring fluid transferringportion or a fluid transferring portion of another system through adetachable connecting flow channel 104. The connecting flow channel 104may be in a form of a tube of which the bilateral ends are connected tothe through holes 100 and 102. Alternatively, the connecting flowchannel 104 may be in a form of a groove formed on a flat thin plate. Inthis case, the flat thin plate may be layered on the bottom surface ofthe base plate 12 to form the connecting flow channel between the bottomsurface of the base plate 12 and an inner surface of the groove.

The micropumps of the cell may be driven with different waveforms asmentioned in the third and fourth modifications of the third embodimentto prevent interference among the three micropumps. Any othermodification mentioned in the previous modifications and embodiments maybe applied to this system.

While the three fluid transferring portions are serially connected inthe example shown in FIG. 33( a), the connections among the fluidtransferring portions can be altered by simply changing the connectingflow channels 104. For instance, left two of the fluid transferringportions may be parallel each other with respect to the most right oneportion by providing connecting flow channels that connect through holes102 and 102 of the left two ones to the through hole 100 of the mostright one. As explained above, the fluid transferring system of FIG. 33(a) has connection flexibility.

FIG. 33( b) shows a bottom view of second another structure of a fluidtransferring system to which the present invention is applicable. Thissystem differ from the system shown in FIG. 33( a) in that the threefluid transferring portions are independently provided on separatecells. Through holes of the cells may be fluidically connected to eachother by detachable connecting flow channels. In this system, theconnecting flow channels may be either of the tube and the flat thinplate. However, in a case where the connecting flow channel is in a formof a groove formed on a flat thin plate, a middle flat plate may beinserted between the flat thin plate and each of the bottom surfaces ofthe base plates of the units to prevent of liquid or gas from leaking.The middle plate preferably has through holes at positions correspondingto the through holes of the cells, and forms U shaped connecting flowchannel together with the flat thin plate. This system has connectionflexibility like as the system shown in FIG. 33( a). Moreover, since thesystem shown in FIG. 33( b) is made up of separate units, the system canbe repaired by simply replace defective unit with new unit.

FIG. 33( c) is a bottom view of third another example of the fluidtransferring system to which the present invention is applicable. Thissystem differ from the system shown in FIG. 33( b) in that no liquidreservoir is provided in each cell, and each of the connecting flowchannels per se has an acoustic capacitance (modulus of elasticity)larger than a predetermined value. Since each of connecting flowchannels has large acoustic capacitance, it can be treated as a pressureabsorbing section. In this system, each cell can be made simple andsmall since no pressure absorbing section is formed in the cell.

Moreover, the present invention is not limited to a liquid, but can beapplied to all kinds of fluids including gases.

A micropump relating to the present invention can be used in variouskinds of application fields, such as environmental preservation, food,biochemistry, immunology, hematology, gene analysis, synthesis, drugdiscovery and others.

Although the present invention has been fully described by way ofexamples with reference to the accompanying drawings, it is to be notedthat various changes and modifications will be apparent to those skilledin the art. Therefore, unless otherwise such changes and modificationsdepart from the scope of the present invention, they should be construedas being included therein.

1. A fluid transferring system comprising: a micropump having a chamber;a first fluid transferring portion connected to the chamber; and asecond fluid transferring portion connected to the chamber, wherein atleast one of the first and second fluid transferring portions comprisesa pressure absorbing section for absorbing or alleviating a liquidvibrational pressure therein and wherein the pressure absorbing sectionis provided across a length ½ or more times a wavelength of a pressurecompressional wave corresponding to a driving cycle of the micropump ina fluid transferring direction of the at least one of first and secondfluid transferring portions.
 2. A fluid transferring system as claimedin claim 1, wherein each of the first and second fluid transferringportions comprises a flow channel or a fluid reservoir.
 3. A fluidtransferring system as claimed in claim 1, wherein the first and secondfluid transferring portions are connected with the chamber throughopening sections provided at the chamber, respectively.
 4. A fluidtransferring system as claimed in claim 1, wherein the first and secondfluid transferring portions are connected with the chamber throughclosing valves, respectively.
 5. A fluid transferring system as claimedin claim 1, wherein the pressure absorbing section comprises a wallsection of which a thickness is thin enough to be deformed by beingapplied the liquid vibrational pressure.
 6. A fluid transferring systemas claimed in claim 5, wherein the wall section forms a portion of theat least one of first and second fluid transferring portions.
 7. A fluidtransferring system as claimed in claim 5, wherein a sum of the absolutevalues of a change in capacity of at least one of the first and secondfluid transferring portions that comprises the pressure absorbingsections caused by deformation when a unit pressure is applied thereto;and change in volume of a liquid residing in the at least one of thefirst and second fluid transferring portions that comprises the pressureabsorbing section when the same unit pressure is applied thereto islarger than the sum of the absolute values of a change in capacity ofthe chamber when a unit pressure is applied thereto and a change involume of the liquid in the chamber when the same unit pressure isapplied thereto.
 8. A fluid transferring system comprising: a micropumphaving a chamber; a first fluid transferring portion connected to thechamber; and a second fluid transferring portion connected to thechamber, wherein at least one of the first and second fluid transferringportions comprises a pressure reflecting section configured to reflect apart of a pressure compressional wave propagating in a direction awayfrom the chamber in the at least one of the first and second fluidtransferring portions back toward the chamber side of the at least oneof the first and second fluid transferring portions.
 9. A fluidtransferring system as claimed in claim 8, wherein each of the first andsecond fluid transferring portions comprises a flow channel or a liquidreservoir.
 10. A fluid transferring system as claimed in claim 8,wherein the first and second fluid transferring portions are connectedwith the chamber through opening sections provided at the chamber,respectively.
 11. A fluid transferring system as claimed in claim 8,wherein the first and second fluid transferring portions are connectedwith the chamber through closing valves, respectively.
 12. A fluidtransferring system as claimed in claim 8, wherein the pressurereflecting section comprises a portion where an effective acousticimpedance is discontinuous.
 13. A fluid transferring system as claimedin claim 8, wherein the pressure reflecting section comprises a flowchannel which bends with a sharp angle.
 14. A fluid transferring systemas in claim 8 wherein the first and second fluid transferring portionsare connected with the chamber through opening sections provided at thechamber, respectively; and wherein a distance from the opening sectionof the micropump to the pressure reflecting section of the at least oneof the first and second fluid transferring portions is shorter than onehalf of the wavelength of a driving cycle of the micropump.
 15. A fluidtransferring system comprising: a micropump having a chamber to which afirst opening section and a second opening section are formed, wherein,when a pressure in the chamber is raised or lowered, a change rate inflow channel resistance at the first opening section is smaller than achange rate in flow channel resistance at the second opening section; afirst fluid transferring portion connected to the chamber though thefirst opening section; and a second fluid transferring portion connectedto the chamber through the second opening section, wherein the firstfluid transferring portion has a reflecting section configured toreflect a part of a pressure compressional wave propagating in adirection away from the chamber in the first fluid transferring portionback toward the chamber side of the first fluid transferring portion.16. A fluid transferring system as claimed in claim 15, wherein adistance in the first fluid transferring portion from the first openingsection to the reflecting section is ½ or less times a wavelength of apressure compressional wave corresponding to a driving cycle of themicropump.
 17. A fluid transferring system comprising: a micropumpcomprising a chamber to which a first opening section and a secondopening section are formed, the chamber having a first capacity,wherein, when a pressure in the chamber is raised or lowered, a changerate in flow channel resistance at the first opening section is smallerthan a change rate in flow channel resistance at the second openingsection; a fluid reservoir connected to the chamber though the firstopening section, the fluid reservoir having a second capacity largerthan the first capacity; a fluid transferring portion connected to thechamber through the second opening section; and wherein the fluidtransferring portion comprises a pressure absorbing section forabsorbing or alleviating a liquid vibrational pressure therein andwherein the pressure absorbing section is provided across a length ½ ormore times a wavelength of a pressure compressional wave correspondingto a driving cycle of the micropump in a fluid transferring direction ofthe at least one of first and second fluid transferring portions.
 18. Afluid transferring system as claimed in claim 17, wherein the fluidtransferring system has no valve.